{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2021:SHFTFUSKEEAM7N2MMJYN26TZOF","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"44900956fa34ed6b1291620192ba97b88db9b066d242788c76c9be446d151a29","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech","cond-mat.str-el"],"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"quant-ph","submitted_at":"2021-11-17T19:00:28Z","title_canon_sha256":"14ae97205794b467b2c9e377ca2f23a32cd364deb602cd13f1e81fb1f6f08ada"},"schema_version":"1.0","source":{"id":"2111.09336","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2111.09336","created_at":"2026-07-05T04:57:23Z"},{"alias_kind":"arxiv_version","alias_value":"2111.09336v1","created_at":"2026-07-05T04:57:23Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2111.09336","created_at":"2026-07-05T04:57:23Z"},{"alias_kind":"pith_short_12","alias_value":"SHFTFUSKEEAM","created_at":"2026-07-05T04:57:23Z"},{"alias_kind":"pith_short_16","alias_value":"SHFTFUSKEEAM7N2M","created_at":"2026-07-05T04:57:23Z"},{"alias_kind":"pith_short_8","alias_value":"SHFTFUSK","created_at":"2026-07-05T04:57:23Z"}],"graph_snapshots":[{"event_id":"sha256:651f2e5585b1d2ec0bb851e4c5d6a03f5c6a21bf64e20e7e506d6d508e73e4b7","target":"graph","created_at":"2026-07-05T04:57:23Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2111.09336/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Monitored quantum circuits (MRCs) exhibit a measurement-induced phase transition between area-law and volume-law entanglement scaling. MRCs with a conserved charge additionally exhibit two distinct volume-law entangled phases that cannot be characterized by equilibrium notions of symmetry-breaking or topological order, but rather by the non-equilibrium dynamics and steady-state distribution of charge fluctuations. These include a charge-fuzzy phase in which charge information is rapidly scrambled leading to slowly decaying spatial fluctuations of charge in the steady state, and a charge-sharp ","authors_text":"Andrew C. Potter, David A. Huse, Fergus Barratt, Romain Vasseur, Sarang Gopalakrishnan, Utkarsh Agrawal","cross_cats":["cond-mat.dis-nn","cond-mat.stat-mech","cond-mat.str-el"],"headline":"","license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"quant-ph","submitted_at":"2021-11-17T19:00:28Z","title":"Field theory of charge sharpening in symmetric monitored quantum circuits"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2111.09336","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:7bb0da3b40d856f9c3cbb0bd73ed769160a48811b9bfe62a376a3b6fd862557a","target":"record","created_at":"2026-07-05T04:57:23Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"44900956fa34ed6b1291620192ba97b88db9b066d242788c76c9be446d151a29","cross_cats_sorted":["cond-mat.dis-nn","cond-mat.stat-mech","cond-mat.str-el"],"license":"http://creativecommons.org/licenses/by-nc-sa/4.0/","primary_cat":"quant-ph","submitted_at":"2021-11-17T19:00:28Z","title_canon_sha256":"14ae97205794b467b2c9e377ca2f23a32cd364deb602cd13f1e81fb1f6f08ada"},"schema_version":"1.0","source":{"id":"2111.09336","kind":"arxiv","version":1}},"canonical_sha256":"91cb32d24a2100cfb74c6270dd7a797164c829de06f973f2e426f8e91a8e153d","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"91cb32d24a2100cfb74c6270dd7a797164c829de06f973f2e426f8e91a8e153d","first_computed_at":"2026-07-05T04:57:23.564093Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T04:57:23.564093Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"g0V1RNgG4WsVCa3cQYVwM56Ek811BdXVT23yBgUrZ9bbteRFaciHNZ3udyl/bJBIvF+DBwEZzzpEaZzCs7IyCA==","signature_status":"signed_v1","signed_at":"2026-07-05T04:57:23.564530Z","signed_message":"canonical_sha256_bytes"},"source_id":"2111.09336","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:7bb0da3b40d856f9c3cbb0bd73ed769160a48811b9bfe62a376a3b6fd862557a","sha256:651f2e5585b1d2ec0bb851e4c5d6a03f5c6a21bf64e20e7e506d6d508e73e4b7"],"state_sha256":"d606f97cda1eef6d03b10754871656a3b9426d0ef8ddcb18c52eefa9364463e0"}